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JP4080486B2 - Method for forming magneto-optical recording medium - Google Patents
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JP4080486B2 - Method for forming magneto-optical recording medium - Google Patents

Method for forming magneto-optical recording medium Download PDF

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JP4080486B2
JP4080486B2 JP2004546387A JP2004546387A JP4080486B2 JP 4080486 B2 JP4080486 B2 JP 4080486B2 JP 2004546387 A JP2004546387 A JP 2004546387A JP 2004546387 A JP2004546387 A JP 2004546387A JP 4080486 B2 JP4080486 B2 JP 4080486B2
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film
dielectric film
magnetic
magnetic film
dielectric
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JPWO2004038717A1 (en
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努 田中
亮 栗田
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Fujitsu Ltd
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    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/1055Disposition or mounting of transducers relative to record carriers
    • G11B11/10576Disposition or mounting of transducers relative to record carriers with provision for moving the transducers for maintaining alignment or spacing relative to the carrier
    • G11B11/10578Servo format, e.g. prepits, guide tracks, pilot signals
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10584Record carriers characterised by the selection of the material or by the structure or form characterised by the form, e.g. comprising mechanical protection elements
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing
    • G11B11/10582Record carriers characterised by the selection of the material or by the structure or form
    • G11B11/10586Record carriers characterised by the selection of the material or by the structure or form characterised by the selection of the material
    • G11B11/10589Details
    • G11B11/10593Details for improving read-out properties, e.g. polarisation of light

Description

この発明は、光磁気記録媒体およびその形成方法に関し、特に、磁壁の移動を利用して再生を行う光磁気記録媒体とその形成方法に関する。  The present invention relates to a magneto-optical recording medium and a method for forming the same, and more particularly, to a magneto-optical recording medium that performs reproduction using movement of a domain wall and a method for forming the same.

従来から、光ビームを照射して情報の記録・再生を行う光磁気記録媒体が実用化されているが、高密度化された記録媒体の再生特性を向上させるために、磁壁の移動を利用した再生方式の光磁気記録媒体が提案されている(例えば、特開平6−290496号公報)。
この文献には、順次積層された3つの磁性層を備え、第1磁性層は上層の第3磁性層に比べて相対的に磁壁抗磁力が小さく、第2磁性層は第1および第3の磁性層よりもキュリー温度が低く、第3磁性層は相対的に磁壁抗磁力が大きく、かつキュリー温度の高い垂直磁化膜である光磁気記録媒体が記載されている。
ここでは、光ビームの照射により第2磁性層のキュリー温度近傍まで温度を上昇させることにより、第1と第3の磁性層との間の交換結合を切断させ、記録マークの境界部の磁壁を温度勾配によって移動させるようにしている。
そして、この磁壁移動により生ずる第1磁性層の磁化反転を、光磁気信号の変化として検出し、情報を再生している。
この再生方法では、記録マークの前方境界部の磁壁と後方境界部の磁壁とが分離独立して形成されていることが、磁壁の移動を安定化し、再生特性を向上させる上で望ましい。
そこで、磁壁の分離を確実なものとするために、従来は磁性膜の成膜後にトラックの両側の案内溝の部分を高出力のレーザーでアニールして、トラック側部の磁性膜を変質もしくは消失させた後に、記録マークを形成することにより、前後の磁壁を分離させるようにしていた。
また、ランドとグルーブの境界の磁壁を分離するために、ランドとグルーブの間の側壁部分に形成された磁性層を酸化した光メモリ素子が提案されている(特開2000−235743号公報参照)。
ここでは、ランド及びグルーブ上の全体にわたって磁性層を形成した後、アルゴンガスを導入した状態で、Siからなる選択酸化層を磁性層の上に形成し、さらに長時間大気中で保持することにより、側壁に形成された磁性層を選択酸化している。
Conventionally, a magneto-optical recording medium that records and reproduces information by irradiating a light beam has been put to practical use. However, in order to improve the reproducing characteristics of a recording medium with a high density, the movement of the domain wall is used. A reproduction-type magneto-optical recording medium has been proposed (for example, Japanese Patent Application Laid-Open No. 6-290496).
This document includes three magnetic layers that are sequentially stacked. The first magnetic layer has a relatively small domain wall coercive force compared to the upper third magnetic layer, and the second magnetic layer includes the first and third magnetic layers. A magneto-optical recording medium is described in which the Curie temperature is lower than that of the magnetic layer, the third magnetic layer has a relatively large domain wall coercive force, and is a perpendicular magnetization film having a high Curie temperature.
Here, by raising the temperature to near the Curie temperature of the second magnetic layer by irradiation with a light beam, the exchange coupling between the first and third magnetic layers is broken, and the domain wall at the boundary portion of the recording mark is It is moved by the temperature gradient.
And the magnetization reversal of the 1st magnetic layer which arises by this domain wall movement is detected as a change of a magneto-optical signal, and information is reproduced.
In this reproducing method, it is desirable that the domain wall at the front boundary part and the domain wall at the rear boundary part of the recording mark are formed separately and independently in order to stabilize the movement of the domain wall and improve the reproduction characteristics.
Therefore, in order to ensure separation of the domain walls, conventionally, after the magnetic film is formed, the guide groove portions on both sides of the track are annealed with a high-power laser to alter or disappear the magnetic film on the track side portion. After that, a recording mark is formed to separate the front and rear domain walls.
In addition, an optical memory element in which a magnetic layer formed on a side wall portion between a land and a groove is oxidized in order to separate a domain wall at the boundary between the land and the groove has been proposed (see Japanese Patent Application Laid-Open No. 2000-235743).
Here, after forming a magnetic layer over the entire land and groove, a selective oxidation layer made of Si is formed on the magnetic layer in a state where argon gas is introduced, and is further maintained in the atmosphere for a long time. The magnetic layer formed on the side wall is selectively oxidized.

発明が解決しようとする課題Problems to be solved by the invention

しかし、従来の文献に記載の光磁気記録媒体では、ディスクの形成後に、一枚一枚のディスクについてレーザアニール処理を行うことが必要であった。したがって、ディスク製造工程が複雑となり、レーザアニール処理をするので、製造安定性も十分ではなく、製造のコストアップになるという問題点があった。また、さらに高密度化が可能ないわゆるランド−グルーブ基板に対しては、この製造方法は適用できないという問題点があった。
また、従来の光メモリ素子では、側壁部分の磁性層を選択酸化させるために、完成媒体には不要な選択酸化層を形成する処理や、その後に長時間大気中に放置しておくか、または酸素ブラズマによる選択酸化処理をする必要があるので、製造工程が複雑で長時間を要し、製造コストのアップの要因となるという問題点があった。
However, in the magneto-optical recording medium described in the conventional literature, it is necessary to perform laser annealing on each disk after the disk is formed. Therefore, the disk manufacturing process becomes complicated and the laser annealing process is performed, so that the manufacturing stability is not sufficient and the manufacturing cost is increased. Further, there is a problem that this manufacturing method cannot be applied to a so-called land-groove substrate which can be further densified.
Further, in the conventional optical memory element, in order to selectively oxidize the magnetic layer on the side wall portion, a process for forming an unnecessary selective oxidation layer on the completed medium, or after being left in the atmosphere for a long time, or oxygen Since it is necessary to perform selective oxidation treatment with plasma, the manufacturing process is complicated and takes a long time, which causes an increase in manufacturing cost.

この発明は、基板上に、少なくとも放熱層を介して、それぞれ組成成分の異なる3層の磁性膜を積層し、これらの構造の上に所定膜厚の誘電体膜を形成した後、情報を記録しない領域の磁性膜を窒化させ、これらの構造の上に前記誘電体膜を構成する材料をさらに積層させてなる光磁気記録媒体の形成方法を提供するものである。
また、基板上に、第1誘電体膜、放熱層、第2誘電体膜をこの順に積層する工程と、前記第2誘電体膜の上に、第1磁性膜と、第1磁性膜よりもキュリー温度の低い第2磁性膜と、第1磁性膜よりも磁壁抗磁力が大きく、かつ第2磁性膜よりもキュリー温度の高い第3磁性膜とをこの順に積層する工程と、前記第3磁性膜の上に、所定膜厚の第4誘電体膜を積層する工程と、情報を記録しない領域の前記第3磁性膜を少なくとも窒化させる工程と、窒化された前記第3磁性膜および第4誘電体膜の上に第3誘電体膜を積層する工程とを含む光磁気記録媒体の形成方法を提供するものである。
これによれば、光磁気記録媒体の製造の容易化および製造コストの削減ができる。
また、この発明は、少なくとも、相対的に磁壁抗磁力が小さな第1磁性膜と、相対的にキュリー温度の低い第2磁性膜と、相対的に磁壁抗磁力が大きく、かつキュリー温度の高い第3磁性膜とをこの順に積層させた光磁気記録媒体であって、少なくとも情報を記録しない領域に存在する前記第3磁性膜が選択的に窒化されていることを特徴とする光磁気記録媒体を提供するものである。
これによれば、光磁気記録媒体の再生特性の安定化およびCNRの向上を図ることができる。
In this invention, three layers of magnetic films having different composition components are laminated on a substrate via at least a heat dissipation layer, and a dielectric film having a predetermined thickness is formed on these structures, and then information is recorded. The present invention provides a method for forming a magneto-optical recording medium in which a magnetic film in a non-performing region is nitrided and a material constituting the dielectric film is further laminated on these structures.
A step of laminating a first dielectric film, a heat dissipation layer, and a second dielectric film in this order on the substrate; and a first magnetic film and a first magnetic film on the second dielectric film. Laminating a second magnetic film having a low Curie temperature and a third magnetic film having a domain wall coercive force larger than that of the first magnetic film and having a Curie temperature higher than that of the second magnetic film in this order; A step of laminating a fourth dielectric film having a predetermined thickness on the film; a step of nitriding at least the third magnetic film in a region where information is not recorded; and the nitrided third magnetic film and fourth dielectric And a method of forming a magneto-optical recording medium including a step of laminating a third dielectric film on the body film.
According to this, manufacturing of the magneto-optical recording medium can be facilitated and manufacturing cost can be reduced.
The present invention also includes at least a first magnetic film having a relatively small domain wall coercivity, a second magnetic film having a relatively low Curie temperature, and a relatively high domain wall coercivity and a high Curie temperature. A magneto-optical recording medium in which three magnetic films are laminated in this order, wherein the third magnetic film existing at least in a region where no information is recorded is selectively nitrided. It is to provide.
According to this, it is possible to stabilize the reproduction characteristics of the magneto-optical recording medium and improve the CNR.

第1図は、この発明の光磁気記録媒体の一実施例の構成図である。
第2図は、この発明の光磁気記録媒体の一実施例の概略断面図である。
第3図は、この発明の光磁気記録媒体の一実施例の製造工程の主要部の説明図である。
第4図は、この発明の光磁気記録媒体において、ランド−グルーブ基板を用いた場合の第4誘電体膜の膜厚とCNRとの関係グラフである。
第5図は、この発明の光磁気記録媒体において、グルーブ基板を用いた場合の第4誘電体膜の膜厚とCNRとの関係グラフである。
第6図は、この発明の光磁気記録媒体において、ランド基板を用いた場合の第4誘電体膜の膜厚とCNRとの関係グラフである。
第7図は、従来の光磁気記録媒体の構成図である。
FIG. 1 is a block diagram of an embodiment of the magneto-optical recording medium of the present invention.
FIG. 2 is a schematic sectional view of an embodiment of the magneto-optical recording medium of the present invention.
FIG. 3 is an explanatory view of the main part of the manufacturing process of one embodiment of the magneto-optical recording medium of the present invention.
FIG. 4 is a graph showing the relationship between the film thickness of the fourth dielectric film and the CNR when a land-groove substrate is used in the magneto-optical recording medium of the present invention.
FIG. 5 is a graph showing the relationship between the film thickness of the fourth dielectric film and the CNR when a groove substrate is used in the magneto-optical recording medium of the present invention.
FIG. 6 is a graph showing the relationship between the film thickness of the fourth dielectric film and the CNR when a land substrate is used in the magneto-optical recording medium of the present invention.
FIG. 7 is a block diagram of a conventional magneto-optical recording medium.

この発明は、光磁気記録媒体において情報を記録する必要のない領域の磁性層を窒化することにより、製造の容易化、製造コストの削減及びCNR特性の向上を図ろうとするものである。
この発明の光磁気記録媒体の形成方法において、前記窒化工程は、第4誘電体膜を積層した後の媒体を室温かつ窒素雰囲気中に所定時間放置すればよい。
また、前記基板としては、表面に交互に複数個のランドおよびグルーブを形成した基板を用いることができ、この場合は、隣接するランドとグルーブとの境界部分が傾斜面からなり、前記傾斜面が情報を記録しない領域であり、この傾斜面には前記第4誘電体膜が積層されない程度に第4誘電体膜がランドおよびグルーブ上の第3磁性膜の上に積層されるようにしてもよい。
また、前記基板として、表面に複数個のグルーブが形成された基板を用いる場合、隣接するグルーブの境界部分が凸形状の側壁面から構成され、前記側壁面が情報を記録しない領域であり、この側壁面には前記第4誘電体膜が積層されない程度に、第4誘電体膜がグルーブ上の第3磁性膜の上に積層されるようにしてもよい。
さらに、前記基板として、表面に複数個のランドが形成された基板を用いる場合、隣接するランドの境界部分が凹形状の側溝から構成され、前記側溝が情報を記録しない領域であり、前記側溝には前記第4誘電体膜が積層されない程度に、第4誘電体膜がランド上の第3磁性膜の上に積層されるようにしてもよい。
この発明において、「磁壁抗磁力」とは、磁性膜の中の磁区の境界に形成されている磁気的な壁を移動させるのに必要な力を言う。たとえば磁気的な壁を移動させにくいものほど、磁壁抗磁力が大きい。
基板上に形成される各層は、スパッタ装置内に配置された各種材料のターゲットをスパッタガスでスパッタリングすることにより形成することができる。
以下、図面に示す実施の形態に基づいてこの発明を詳述する。なお、これによってこの発明が限定されるものではない。
〈光磁気記録媒体の構成〉
図1に、この発明の光磁気記録媒体の一実施例の構成図を示す。
図1に示すように、この発明の光磁気記録媒体は、
基板1の上に、第1誘電体膜2、放熱層3、第2誘電体膜4、第1磁性膜5、第2磁性膜6、第3磁性膜7、第4誘電体膜81、および第3誘電体膜82を、この順に形成したものである。
以下に、各層の膜厚および材料の一実施例を示す。
基板1:1.2mm;ガラス
第1誘電体膜2:5nm;SiN
放熱層3:30nm;Ag
第2誘電体膜4:30nm;SiN
第1磁性膜5:60nm;Tb27Fe57Co16
第2磁性膜6:10nm;Tb20Fe79Co
第3磁性膜7:30nm;Gd27Fe62Co11
第4誘電体膜81:2nm;SiN
第3誘電体膜82:53nm;SiN
上記各層の材料は、一実施例であり、必要に応じて他の材料を採用してもよい。また、この実施例の媒体は基板とは異なる第3誘電体膜82側から光を照射するタイプの媒体(フロントサーフェス媒体)である。
もちろん、この発明の媒体構成は、通常用いられている基板1側から光を入射させるタイプの媒体にも適用できるが、この場合には、第1磁性膜5と第3磁性膜7の材料及び膜厚は逆にする。
なお、第3誘電体膜側から光を照射するフロントサーフェス媒体は、膜厚の厚い基板を介さずに光が磁性膜に届くので、対物レンズを小さくでき、基板側から光を照射する媒体よりも高密度化することができる。
この発明の基板1としては、ガラスの他、Al合金や、SiなどのHDD(Hard Disk Drive)用材料を用いてもよい。
第1誘電体膜2としては、C,SiO,Y−SiO,AlNなどでもよい。
第2誘電体膜4としては、C,SiO,Y−SiO,ZnSiO,AlO,AlNなどの酸化物あるいは窒化物を用いてもよい。
第3および第4誘電体膜81,82としては、SiO,ZnSiO,AlO,AlNなどの酸化物あるいは窒化物を用いてもよい。
放熱層3としては、AlTi,AlCrなどのAl合金や、Ag、Au,Pt及びこれらの金属を主成分とした合金などを用いてもよい。
第1磁性膜5は、TbFeCoの他、DyFeCo,TbDyFeCoなどの希土類−遷移金属を用いてもよい。
第2磁性膜6は、TbFeCoの他、DyFeCo,TbDyFeCoなどの希土類−遷移金属を用いてもよい。
第3磁性膜7は、GdFeCoの他、GdFeCoAl,GdTbFeCo,GdDyFeCoなどの希土類−遷移金属を用いてもよい。
ここで、第1磁性膜5は、第3磁性膜7よりも相対的に磁壁抗磁力が高くなるように材料および組成を選択する。
また、第2磁性膜6は、そのキュリー温度が第1および第3磁性膜(5,7)よりも低くなるように、材料および組成を選択する。
また、第3磁性膜7は、第1および第2磁性膜(5,6)よりも、磁壁抗磁力が低く、キュリー温度が高くなるように、材料および組成を選択する。
図1において、第3および第4誘電体膜(81,82)は、いずれもSiNであり、膜厚が異なるだけである。
ただし、後述するように、比較的薄い第4誘電体膜81を形成し、第1〜第3磁性層(5,6,1)を窒化する処理を実行した後に、第3誘電体膜82を形成する。第3および第4誘電体膜を一度に形成してしまわないのは、55nm程度の厚い誘電体膜を磁性膜の上に形成すると、その下層の磁性膜の十分な窒化ができないからである。
また、第4誘電体膜81の膜厚は、情報を記録しない領域には形成されず、情報を記録する領域のCNRを十分確保しつつ、情報を記録する領域の磁性層は窒化されない程度の厚さとする。このために、第4誘電体膜81の膜厚は、1〜10nmの範囲内とすることが好ましい。
また、エンハンスメントのために、第4誘電体膜81と第3誘電体膜82との合計膜厚が55nm程度となるように、両誘電体膜の膜厚を調整すればよい。さらに、光学,熱的な条件調整のためにはこの合計膜厚を調整すればよい。
図1に示したこの発明の光磁気記録媒体は、基板として、(a)ランド−グルーブ基板、(b)グルーブ基板、(c)ランド基板のいずれにも適用できる。特に、従来の媒体のように、レーザアニール処理をしていた場合には、ランドまたはグルーブ上の磁性層を消失させていたので、(a)ランド−グルーブ基板は使用できなかったが、この発明では、(a)ランド−グルーブ基板も使用できるので、高密度の光磁気記録媒体を提供することができる。
図2に、この発明の一実施例において、3つの基板に形成した光磁気記録媒体の概略断面図を示す。
ここでは、説明のため、図1に示した第1誘電体膜2から第3磁性膜7までを区別して表示していないが、実際には層構造が形成されている。
また、第3磁性層7の上に、第4および第3誘電体膜(81,82)が形成されるが、正確な膜厚を反映した図面ではない。
図2(a)は、ランド−グルーブ基板の場合を示しているが、ランド21およびグルーブ22の平坦な部分が情報の記録領域であり、この領域のランド21とグルーブ22に形成された磁性膜(5,6,7)で情報が記録・再生される。
また、ランド21とグルーブ22との境界部分、すなわち図2(a)に示した傾斜面の領域Aおよび領域Bの磁性膜(5,6,7)は窒化処理されており、情報が記録・再生されない領域である。情報が記録・再生されない領域A,Bが窒化されているので、ランド21の情報記録領域と、グルーブ22の情報記録領域とが磁気的に分離され、情報の再生時の信頼性を向上させることができる。
図2(b)は、グルーブ基板であるが、凸形状の側壁面の部分の基板表面に形成された領域Aおよび領域Bの中の磁性膜を窒化することにより、隣接するグルーブ22の平坦部分が磁気的に分離される。
図2(b)では、グルーブ22の平坦部分(トラックピッチ0.4μm程度)が情報の記録領域であり、凸形状の側壁面は記録領域としては用いられず、サーボトラックのために用いられる。
図2(c)は、ランド基板であるが、凹形状の側溝に形成された領域Aおよび領域Bの中の磁性膜(5,6,7)を窒化することにより、隣接するランド21の平坦部分が磁気的に分離される。
図2(c)では、ランド21の平坦部分(トラックピッチ0.4μm程度)が情報の記録領域であり、凹形状の側溝は記録領域としては用いられず、サーボトラックのために用いられる。
〈光磁気記録媒体の形成方法〉
次に、この発明の一実施例の媒体の各層の形成方法を説明する。
まず、図2に示したようないずれかの表面形状を持つ基板1を作成する。ここで、基板1は、金属やPC(ポリカーボネート)などのプラスチックを用いて形成することができる。
次に、図1に示した基板上の各層(2〜82)を形成するために、DCマグネトロンスパッタ装置内の所定の位置に基板1を設置する。
そして、各層を形成するのに必要なターゲットを、基板1と対向する位置に配置し、Arガス等の反応性ガス雰囲気中で反応性スパッタを順次行う。
反応性スパッタは、自公転しながらターゲットの近傍を回転するテーブルに基板1を設置して行うか、または基板を固定したままターゲットを回転させながら行う。また、反応性スパッタは、室温で行う。
図3に、この発明の第1実施例の光磁記記録媒体の形成工程の主要部について示す。
図3では、ランド−グルーブ基板を用いた場合の断面構造を示しているが、グルーブ基板およびランド基板でも形成工程の順序および条件は同様である。基板の表面形状が異なるために、積層構造は異なるが、窒化される領域はいずれも記録されない領域である。
第1実施例の各層の形成は、次の順序で行う。
〔工程1〕第1誘電体膜2の形成
ターゲット:Si
スパッタガス:Arガス、Nガス
流量比:Ar:N=2:1
ガス圧:0.3Pa
投入電力:0.5kw
上記条件のもとで、第1誘電体膜2としてのSiNを、基板1上に膜厚5nm程度形成する。
〔工程2〕放熱層3の形成
ターゲット:Ag
スパッタガス:Arガス
ガス圧:0.1Pa
投入電力:0.5kw
上記条件のもとで、放熱層3としてのAg膜を、第1誘電体膜2の上に、膜厚30nm程度形成する。
〔工程3〕第2誘電体膜4の形成
ターゲット:Si
スパッタガス:Arガス、Nガス
流量比:Ar:N=2:1
ガス圧:0.3Pa
投入電力:0.5kw
上記条件のもとで、第2誘電体膜4としてのSiNを、放熱層3の上に、膜厚30nm程度形成する。
〔工程4〕第1磁性膜5の形成
ターゲット:Tb27Fe57Co16の合金ターゲット
スパッタガス:Arガス
ガス圧:0.5Pa
投入電力:0.5kw
上記条件のもとで、第1磁性膜5としてのTb27Fe57Co16を、第2誘電体膜4の上に、膜厚60nm程度形成する。ここで、第1磁性膜5のキュリー温度は260度となり、次に形成される第2磁性膜6よりも高い温度である。
〔工程5〕第2磁性膜6の形成
ターゲット:Tb20Fe79Co1の合金ターゲット
スパッタガス:Arガス
ガス圧:0.5Pa
投入電力:0.5kw
上記条件のもとで、第2磁性膜6としてのTb20Fe79Co1を、第1磁性膜5の上に、膜厚10nm程度形成する。ここで、第2磁性膜6のキュリー温度は130度程度で、第1および第3磁性膜(5,7)よりも低い。
〔工程6〕第3磁性膜7の形成
ターゲット:Gd27Fe62Co11の合金ターゲット
スパッタガス:Arガス
ガス圧:0.5Pa
投入電力:0.5kw
上記条件のもとで、第3磁性膜7としてのGd27Fe62Co11を、第2磁性層6の上に、膜厚30nm程度形成する。ここで、第3磁性膜7のキュリー温度は240度となり、第2磁性膜6よりも高い。
なお、第1、第2および第3磁性膜の組成比は、上記組成比に限定するものではなく、第1および第3磁性膜(5,7)のキュリー温度が第2磁性膜6のキュリー温度よりも高くなり、磁壁移動タイプとなるように、各磁性層の組成比を選択すればよい。
図3(a)は、基板1上に、第1誘電体膜2から第3磁性膜7までを形成した後の概略断面図を示している。ここで、ランドとグルーブの境界部分、すなわち情報を記録しない部分にも磁性膜(5,6,7)が形成されているが、この境界部分は、傾斜面となっているので、情報を記録するランド21およびグルーブ22の平坦部分よりも薄い膜厚で形成される。
傾斜面で磁性膜等の膜厚が薄くなるのは、反応性スパッタをするときのスパッタ粒子の指向性によるものと考えられる。一般に、マグネトロンスパッタ装置では、基板の平坦部分に均一に製膜するために、スパッタ粒子は、基板上方から基板に対して垂直に飛来するようにしている。すなわち、垂直方向の指向性の強いスパッタ装置では、傾斜面に付着することの多い斜め方向に飛来する粒子の数は少ないので、傾斜面の膜厚は薄くなる。
〔工程7〕第4誘電体膜81の形成
ターゲット:Si
スパッタガス:Arガス、Nガス
流量比:Ar:N=2:1
ガス圧:0.3Pa
投入電力:0.5kw
上記条件のもとで、第4誘電体膜81としてのSiNを、第3磁性膜7の上に、膜厚2nm程度形成する。ここで、第4誘電体膜81の膜厚は、次の窒化処理で、隣接する記録領域が磁気的に分離される程度に、記録領域でない部分の磁性膜(5,6,7)が十分に窒化されるように、選択する必要があり、2nmに限るものではない。
第4誘電体膜81も、境界部分の傾斜面にいくらか積層されるが、前記したようなスパッタ装置の垂直指向性のために、傾斜面上ではランドおよびグルーブの平坦部分に比べて、かなり薄く形成される。
また、第4誘電体膜81を形成するときに、スパッタ粒子の垂直方向の指向性を厳密に管理し、かつ基板の傾斜角を最適化した条件のもとでは、第4誘電体膜81を形成するスパッタ粒子が、傾斜面にはほとんど付着しないように制御できる。
図3(b)は、第4誘電体膜81を形成した後の断面図を示している。同図に示すように、第4誘電体膜81は、他の層(2〜7)と同様に、ランド21およびグルーブ22の平坦部分に形成されるが、ランドとグルーブの境界部分(傾斜面)にはほとんど形成されないようにできる。このため、次の工程8の窒化処理では、第4誘電体膜81が形成されない境界部分、すなわち傾斜面の部分の磁性膜が窒化される。
なお、後述するように、従来の光磁気記録媒体と同等か、それ以上のCNRを確保するためには、第4誘電体膜81の膜厚を数nm程度(1〜10nm)とすることが好ましい。特に、例えばランド−グルーブ基板であれば、45dB以上のCNRを得るためには、第4誘電体膜81の膜厚は、2〜5nm程度が良い。
〔工程8〕磁性膜の窒化処理
工程7の後の媒体について、ガス圧1.0PaのNガスをスパッタ装置の中に導入し、室温で5分間程度放置することにより、窒化処理を行う。
ここで、各磁性膜(5,6,7)は、例えば、ランド−グルーブ基板の平坦部分と境界部分のどちらにも積層されているが、境界部分は傾斜面となっているので、各磁性膜の膜厚は、平坦部分よりも薄い。また、境界部分には第4誘電体膜は積層されない。したがって、膜厚の薄い境界部分(図2の領域A,B)の磁性膜が、窒化されることになる。
また、あまりに長時間Nガスの雰囲気中に媒体をさらすと、窒化してほしくない記録領域の部分も窒化が進行してしまう。
そこで、ランド−グルーブ基板のランドとグルーブの境界部分(傾斜面)、グルーブ基板の凸形状の側壁面、またはランド基板の凹形状の側溝の領域のみが窒化される程度の時間だけ放置することが好ましいので、放置時間は5分に限るものではない。
図3(c)は、窒化処理をした後の断面図を示している。この窒化処理により、ランド21とグルーブ22の境界部分に存在する磁性膜(5,6,7)が窒化され、窒化膜25,26が形成される。
この窒化膜25,26の部分では、磁性が消失しているので、情報は記録できない。したがって、隣接するランド21の平坦部分とグルーブ22の平坦部分の磁性膜(5,6,7)は、窒化膜25,26によって磁気的に分離される。
また、磁性膜は、3つの層(5,6,7)からなるが、隣接する記録領域の磁性膜を磁気的に分離するためには、少なくとも第3磁性膜7を窒化すればよい。したがって、積層された磁性膜(5,6,7)および第4誘電体膜81の膜厚や、要求される記録特性等を考慮して、適切な放置時間を選択すればよい。
〔工程9〕第3誘電体膜82の形成
ターゲット:Si
スパッタガス:Arガス、Nガス
流量比:Ar:N=2:1
ガス圧:0.3Pa
投入電力:0.5kw
上記条件のもとで、第3誘電体膜82としてのSiNを、第4誘電体膜81の上に、膜厚53nm程度形成する。ここで、膜厚は53nmに限るものではなく、第4誘電体膜81の膜厚との合計が55nm程度となるように設定すればよい。
第4誘電体膜81を1〜10nmの間で形成したとすると、第3誘電体膜82は54〜45nm程度形成すればよい。
以上の工程1〜9により、図3(d)に示すようなこの発明の光磁気記録媒体が完成される。
この形成工程では、従来のようにレーザアニールという工程を含まず、窒化処理を除く全ての工程が室温で行う反応性スパッタであるので、形成工程をスムーズに進行させることができ、製造コストを削減することができる。また、酸化処理のように後で再生特性が劣化することもなく、安定性の高い再生を行うことができる。
〈光磁気記録媒体の再生特性〉
次に、この発明の光磁気記録媒体の再生特性について説明する。
再生特性を調べるために、次のような評価実験を行った。
評価装置:スペクトルアナライザー
光学系:対物レンズNA=0.85、波長405nm
記録:レーザストローブ磁界変調記録方式
記録周波数50MHz(=0.15μm)
評価値:CNR(信号対雑音比dB)
比較のために、図7に示した従来の媒体で、第3磁性膜7の形成後に記録しない領域の磁性膜をレーザアニールしたものと、レーザアニールしないで、第3誘電体膜8を形成したものを作成した。
レーザアニールをした従来の媒体としては、グルーブ基板とランド基板を用い、レーザアニールをしない従来の媒体としては、ランド−グルーブ基板を含む3種類の基板を用いた。
また、従来の媒体において、基板1に形成する第1誘電体膜2から第3磁性層7までは、この発明の形成工程のうち工程1から工程6に示したのと同一の条件および同一の膜厚で形成した。第3誘電体膜8は、工程9と同一の条件で膜厚が53nmとなるように形成した。
レーザアニールをする場合は、第3誘電体膜8の形成前に第3磁性層7の記録をしない領域に対して、高出力のレーザを照射してレーザアニールを行った。
また、この発明の媒体において、窒化処理の効果を確認するために、窒化処理の時間を5分間に固定し、第4誘電体膜81の膜厚を1nmから10nmまで1nm単位で変化させたものをそれぞれ作成した。
図4に、ランド−グルーブ基板を用いた場合のこの発明の媒体の再生時におけるCNR(dB)、図5に、グルーブ基板を用いた場合のCNR(dB)、図6に、ランド基板を用いた場合のCNR(dB)を示す。いずれも、横軸は第4誘電体膜81の膜厚(nm)である。
(a)ランド−グルーブ基板の再生特性
まず、ランド−グルーブ基板の場合、レーザアニールをしない従来の媒体は、磁壁が分離されていないため、再生時に磁区拡大は生じず、再生不良となった。
一方、この発明の媒体では、図4に示すように第4誘電体膜81の膜厚が1nmおよび10nmの場合には、CNRは37dB程度で若干悪いが、2nmから7nmの範囲内では、CNR=42〜46dBの範囲内にあり、実用的な数値を示した。
特に、第4誘電体膜81の膜厚を2nmとしたとき、CNR=45.5dBを示しており、磁区拡大が十分に行われ、窒化の効果が最も大きかった。
第4誘電体膜81の膜厚が1nm程度以下では、記録領域であるランドおよびグルーブの平坦部分も窒化されている可能性が高いので、CNRが低くなると考えられる。
また、10nm以上の膜厚になると、ランドとグルーブの境界部分である傾斜面にも第4誘電体膜81が積層されていると考えられ、この境界部分の窒化処理が不十分となったために、磁性膜の分離が不完全となり、CNRが低くなると考えられる。
したがって、ランド−グルーブ基板の場合、第4誘電体膜81の膜厚を2nmから7nmの範囲の適切な数値を選べば、再生時に安定した磁区拡大が生じ、実用上良好なCNRを得ることができる。
(b)グルーブ基板の再生特性
次に、グルーブ基板の場合、レーザアニールをしない従来の媒体では、再生時の磁区拡大は生じず、再生不良となった。
また、レーザアニールをした従来の媒体では、磁区拡大による再生が可能であり、CNRは43.0dBであった。
一方、この発明の媒体では、図5に示すように、第4誘電体膜81の膜厚が2〜5nmの範囲で、従来の媒体のCNRよりも高いCNRを示した。特に、図5によれば、膜厚が3nmの時に、CNR=46.0dBとなり、窒化の効果が最も大きかった。
したがって、グルーブ基板の場合も、この発明の媒体の第4誘電体81の膜厚を適切に選べば、再生時に安定した磁区拡大が生じ、実用上良好なCNRを得ることができる。
(c)ランド基板の再生特性
次に、ランド基板の場合、レーザアニールをしない従来の媒体では、再生時の磁区拡大は生じず、再生不良となった。
また、レーザアニールをした従来の媒体では、磁区拡大による再生が可能であり、CNRは42.5dBであった。
一方、この発明の媒体では、図6に示すように、第4誘電体膜81の膜厚が2〜6nmの範囲で、従来の媒体のCNRよりも高いCNRを得た。特に、図6によれば、膜厚が3nmの時に、CNR=45.5dBとなり、窒化の効果が最も大きかった。
したがって、ランド基板の場合も、第4誘電体膜81の膜厚を適切に選べば、再生時に安定した磁区拡大が生じ、実用上良好なCNRを得ることができる。
このように、この発明の光磁気記録媒体では、積層された磁性膜の上に、所定膜厚の誘電体膜を形成した後に、情報の記録領域ではない部分の磁性膜を窒化させているので、安定した再生特性を有し、実用上良好なCNRを得ることができる。
また、従来の媒体のように、レーザアニールという工程をする必要がないので、製造工程の容易化、製造コストの削減をすることができ、窒化処理をして磁壁の分離をしているので、再生特性がより安定しかつ劣化のない光磁気記録媒体を提供できる。
さらに、この発明の積層構造の媒体は、ランド−グルーブ基板にも適応でき、高密度媒体における製造コストの削減と再生特性を向上できる。
The present invention intends to facilitate manufacturing, reduce manufacturing cost, and improve CNR characteristics by nitriding a magnetic layer in a region where information is not required to be recorded in a magneto-optical recording medium.
In the method for forming a magneto-optical recording medium according to the present invention, the nitriding step may be performed by leaving the medium after the fourth dielectric film is laminated in a nitrogen atmosphere at room temperature for a predetermined time.
Further, as the substrate, a substrate in which a plurality of lands and grooves are alternately formed on the surface can be used. In this case, a boundary portion between adjacent lands and grooves is an inclined surface, and the inclined surface is It is an area where information is not recorded, and the fourth dielectric film may be laminated on the third magnetic film on the land and the groove to the extent that the fourth dielectric film is not laminated on the inclined surface. .
Further, when a substrate having a plurality of grooves formed on the surface is used as the substrate, the boundary portion between adjacent grooves is constituted by a convex side wall surface, and the side wall surface is an area where information is not recorded. The fourth dielectric film may be laminated on the third magnetic film on the groove to the extent that the fourth dielectric film is not laminated on the side wall surface.
Further, when a substrate having a plurality of lands formed on the surface is used as the substrate, the boundary portion between adjacent lands is composed of concave side grooves, and the side grooves are areas where information is not recorded, and the side grooves The fourth dielectric film may be laminated on the third magnetic film on the land so that the fourth dielectric film is not laminated.
In the present invention, the “domain wall coercive force” refers to a force required to move a magnetic wall formed at the boundary between magnetic domains in the magnetic film. For example, the harder the magnetic wall is moved, the greater the domain wall coercivity.
Each layer formed on the substrate can be formed by sputtering a target of various materials arranged in a sputtering apparatus with a sputtering gas.
The present invention will be described in detail below based on the embodiments shown in the drawings. However, this does not limit the present invention.
<Configuration of magneto-optical recording medium>
FIG. 1 shows a block diagram of an embodiment of the magneto-optical recording medium of the present invention.
As shown in FIG. 1, the magneto-optical recording medium of the present invention is
On the substrate 1, a first dielectric film 2, a heat dissipation layer 3, a second dielectric film 4, a first magnetic film 5, a second magnetic film 6, a third magnetic film 7, a fourth dielectric film 81, and A third dielectric film 82 is formed in this order.
An example of the film thickness and material of each layer is shown below.
Substrate 1: 1.2 mm; glass first dielectric film 2: 5 nm; SiN
Heat dissipation layer 3: 30 nm; Ag
Second dielectric film 4: 30 nm; SiN
First magnetic film 5: 60 nm; Tb 27 Fe 57 Co 16
Second magnetic film 6: 10 nm; Tb 20 Fe 79 Co 1
Third magnetic film 7: 30 nm; Gd 27 Fe 62 Co 11
Fourth dielectric film 81: 2 nm; SiN
Third dielectric film 82: 53 nm; SiN
The material of each of the above layers is an example, and other materials may be adopted as necessary. The medium of this embodiment is a medium (front surface medium) that irradiates light from the third dielectric film 82 side, which is different from the substrate.
Of course, the medium configuration of the present invention can also be applied to a type of medium in which light is incident from the normally used substrate 1 side. In this case, the materials of the first magnetic film 5 and the third magnetic film 7 and The film thickness is reversed.
The front surface medium that irradiates light from the third dielectric film side can reach the magnetic film without going through the thick substrate, so that the objective lens can be made smaller than the medium that irradiates light from the substrate side. Can also be densified.
As the substrate 1 of the present invention, in addition to glass, a material for HDD (Hard Disk Drive) such as an Al alloy or Si may be used.
As the first dielectric layer 2, C, SiO 2, Y -SiO 2, AlN or the like.
As the second dielectric film 4, oxides or nitrides such as C, SiO 2 , Y—SiO 2 , ZnSiO 2 , AlO, and AlN may be used.
As the third and fourth dielectric films 81 and 82, oxides or nitrides such as SiO 2 , ZnSiO 2 , AlO, and AlN may be used.
As the heat dissipation layer 3, an Al alloy such as AlTi and AlCr, an alloy mainly composed of Ag, Au, Pt, and these metals may be used.
The first magnetic film 5 may use rare earth-transition metals such as DyFeCo and TbDyFeCo in addition to TbFeCo.
The second magnetic film 6 may use a rare earth-transition metal such as DyFeCo and TbDyFeCo in addition to TbFeCo.
The third magnetic film 7 may use a rare earth-transition metal such as GdFeCoAl, GdTbFeCo, GdDyFeCo in addition to GdFeCo.
Here, the material and composition of the first magnetic film 5 are selected so that the domain wall coercive force is relatively higher than that of the third magnetic film 7.
The material and composition of the second magnetic film 6 are selected so that the Curie temperature is lower than that of the first and third magnetic films (5, 7).
The material and composition of the third magnetic film 7 are selected so that the domain wall coercive force is lower and the Curie temperature is higher than those of the first and second magnetic films (5, 6).
In FIG. 1, the third and fourth dielectric films (81, 82) are both SiN and differ only in film thickness.
However, as will be described later, the third dielectric film 82 is formed after the relatively thin fourth dielectric film 81 is formed and the first to third magnetic layers (5, 6, 1) are nitrided. Form. The reason why the third and fourth dielectric films are not formed at a time is that when a thick dielectric film of about 55 nm is formed on the magnetic film, the underlying magnetic film cannot be sufficiently nitrided.
Further, the film thickness of the fourth dielectric film 81 is not formed in the area where information is not recorded, and the magnetic layer in the area where information is recorded is not nitrided while sufficiently ensuring the CNR of the area where information is recorded. Thickness. For this reason, the thickness of the fourth dielectric film 81 is preferably in the range of 1 to 10 nm.
For enhancement, the thicknesses of both dielectric films may be adjusted so that the total thickness of the fourth dielectric film 81 and the third dielectric film 82 is about 55 nm. Further, the total film thickness may be adjusted for adjusting optical and thermal conditions.
The magneto-optical recording medium of the present invention shown in FIG. 1 can be applied to any of (a) land-groove substrate, (b) groove substrate, and (c) land substrate. In particular, when the laser annealing treatment was performed as in the conventional medium, the magnetic layer on the land or groove was lost, so (a) the land-groove substrate could not be used. Then, since (a) a land-groove substrate can be used, a high-density magneto-optical recording medium can be provided.
FIG. 2 is a schematic sectional view of a magneto-optical recording medium formed on three substrates in one embodiment of the present invention.
Here, for the sake of explanation, the first dielectric film 2 to the third magnetic film 7 shown in FIG. 1 are not distinguished from each other, but a layer structure is actually formed.
Further, although the fourth and third dielectric films (81, 82) are formed on the third magnetic layer 7, this is not a drawing reflecting an accurate film thickness.
FIG. 2A shows the case of a land-groove substrate. The flat portions of the land 21 and the groove 22 are information recording areas, and the magnetic film formed on the land 21 and the groove 22 in this area. Information is recorded / reproduced at (5, 6, 7).
Further, the boundary portion between the land 21 and the groove 22, that is, the magnetic films (5, 6, 7) in the inclined surface area A and area B shown in FIG. This area is not played back. Since the areas A and B where information is not recorded / reproduced are nitrided, the information recording area of the land 21 and the information recording area of the groove 22 are magnetically separated, and the reliability at the time of reproducing information is improved. Can do.
FIG. 2B shows a groove substrate, but a flat portion of the adjacent groove 22 is formed by nitriding the magnetic film in the region A and the region B formed on the surface of the convex side wall surface portion. Are magnetically separated.
In FIG. 2B, the flat portion of the groove 22 (track pitch of about 0.4 μm) is an information recording area, and the convex side wall surface is not used as a recording area but is used for a servo track.
FIG. 2C shows a land substrate. By nitriding the magnetic films (5, 6, 7) in the regions A and B formed in the concave side grooves, the adjacent lands 21 are flattened. The parts are magnetically separated.
In FIG. 2C, the flat portion of the land 21 (track pitch of about 0.4 μm) is an information recording area, and the concave side groove is not used as a recording area but is used for a servo track.
<Method of forming magneto-optical recording medium>
Next, a method for forming each layer of the medium according to the embodiment of the present invention will be described.
First, a substrate 1 having any surface shape as shown in FIG. 2 is prepared. Here, the board | substrate 1 can be formed using plastics, such as a metal and PC (polycarbonate).
Next, in order to form each layer (2-82) on the substrate shown in FIG. 1, the substrate 1 is set at a predetermined position in the DC magnetron sputtering apparatus.
Then, a target necessary for forming each layer is disposed at a position facing the substrate 1, and reactive sputtering is sequentially performed in a reactive gas atmosphere such as Ar gas.
Reactive sputtering is performed by placing the substrate 1 on a table that rotates in the vicinity of the target while revolving, or while rotating the target while the substrate is fixed. Reactive sputtering is performed at room temperature.
FIG. 3 shows the main part of the formation process of the magneto-optical recording medium of the first embodiment of the present invention.
Although FIG. 3 shows a cross-sectional structure when a land-groove substrate is used, the order and conditions of the forming steps are the same for the groove substrate and the land substrate. Since the surface shapes of the substrates are different, the laminated structure is different, but the areas to be nitrided are all areas that are not recorded.
Each layer of the first embodiment is formed in the following order.
[Step 1] Formation of first dielectric film 2 Target: Si
Sputtering gas: Ar gas, N 2 gas Flow rate ratio: Ar: N 2 = 2: 1
Gas pressure: 0.3Pa
Input power: 0.5 kW
Under the above conditions, SiN as the first dielectric film 2 is formed on the substrate 1 with a thickness of about 5 nm.
[Step 2] Formation of heat dissipation layer 3 Target: Ag
Sputtering gas: Ar gas Gas pressure: 0.1 Pa
Input power: 0.5 kW
Under the above conditions, an Ag film as the heat dissipation layer 3 is formed on the first dielectric film 2 with a thickness of about 30 nm.
[Step 3] Formation of second dielectric film 4 Target: Si
Sputtering gas: Ar gas, N 2 gas Flow rate ratio: Ar: N 2 = 2: 1
Gas pressure: 0.3Pa
Input power: 0.5 kW
Under the above conditions, SiN as the second dielectric film 4 is formed on the heat dissipation layer 3 with a thickness of about 30 nm.
[Step 4] Formation of the first magnetic film 5 Target: Alloy target of Tb27Fe57Co16 Sputtering gas: Ar gas Gas pressure: 0.5 Pa
Input power: 0.5 kW
Under the above conditions, Tb27Fe57Co16 as the first magnetic film 5 is formed on the second dielectric film 4 to a thickness of about 60 nm. Here, the Curie temperature of the first magnetic film 5 is 260 degrees, which is higher than the second magnetic film 6 to be formed next.
[Step 5] Formation of second magnetic film 6 Target: Alloy target of Tb20Fe79Co1 Sputtering gas: Ar gas Gas pressure: 0.5 Pa
Input power: 0.5 kW
Under the above conditions, Tb20Fe79Co1 as the second magnetic film 6 is formed on the first magnetic film 5 to a thickness of about 10 nm. Here, the Curie temperature of the second magnetic film 6 is about 130 degrees, which is lower than that of the first and third magnetic films (5, 7).
[Step 6] Formation of third magnetic film 7 Target: Alloy target of Gd27Fe62Co11 Sputtering gas: Ar gas Gas pressure: 0.5 Pa
Input power: 0.5 kW
Under the above conditions, Gd27Fe62Co11 as the third magnetic film 7 is formed on the second magnetic layer 6 with a film thickness of about 30 nm. Here, the Curie temperature of the third magnetic film 7 is 240 degrees, which is higher than that of the second magnetic film 6.
The composition ratio of the first, second, and third magnetic films is not limited to the above composition ratio, and the Curie temperature of the first and third magnetic films (5, 7) is the Curie of the second magnetic film 6. What is necessary is just to select the composition ratio of each magnetic layer so that it becomes higher than temperature and becomes a domain wall motion type.
FIG. 3A shows a schematic cross-sectional view after the first dielectric film 2 to the third magnetic film 7 are formed on the substrate 1. Here, the magnetic film (5, 6, 7) is also formed at the boundary portion between the land and the groove, that is, the portion where information is not recorded. However, since this boundary portion is an inclined surface, information is recorded. The land 21 and the groove 22 are formed with a film thickness thinner than the flat portions.
The thin film thickness of the magnetic film or the like on the inclined surface is considered to be due to the directivity of the sputtered particles when reactive sputtering is performed. In general, in a magnetron sputtering apparatus, in order to uniformly form a film on a flat portion of a substrate, sputtered particles fly vertically from above the substrate. That is, in a sputtering apparatus having a strong vertical directivity, the number of particles that frequently fly on the inclined surface and fly in an oblique direction is small, so that the thickness of the inclined surface becomes thin.
[Step 7] Formation of fourth dielectric film 81 Target: Si
Sputtering gas: Ar gas, N 2 gas Flow rate ratio: Ar: N 2 = 2: 1
Gas pressure: 0.3Pa
Input power: 0.5 kW
Under the above conditions, SiN as the fourth dielectric film 81 is formed on the third magnetic film 7 to a thickness of about 2 nm. Here, the thickness of the fourth dielectric film 81 is such that the portion of the magnetic film (5, 6, 7) that is not the recording area is sufficiently large that the adjacent recording area is magnetically separated by the next nitriding process. It is necessary to select such that it is nitrided to 1 nm, and it is not limited to 2 nm.
The fourth dielectric film 81 is also somewhat laminated on the inclined surface of the boundary portion. However, due to the vertical directivity of the sputtering apparatus as described above, the fourth dielectric film 81 is considerably thinner on the inclined surface than the flat portion of the land and groove. It is formed.
Further, when the fourth dielectric film 81 is formed, the fourth dielectric film 81 is formed under the condition that the directivity in the vertical direction of the sputtered particles is strictly controlled and the tilt angle of the substrate is optimized. It can control so that the sputtered particle to form hardly adheres to an inclined surface.
FIG. 3B shows a cross-sectional view after the fourth dielectric film 81 is formed. As shown in the figure, the fourth dielectric film 81 is formed on the flat portion of the land 21 and the groove 22 like the other layers (2 to 7), but the boundary portion between the land and the groove (inclined surface). ) Can hardly be formed. For this reason, in the nitriding process in the next step 8, the boundary portion where the fourth dielectric film 81 is not formed, that is, the magnetic film at the inclined surface portion is nitrided.
As will be described later, in order to ensure a CNR equal to or higher than that of a conventional magneto-optical recording medium, the thickness of the fourth dielectric film 81 is set to about several nm (1 to 10 nm). preferable. In particular, in the case of a land-groove substrate, for example, the thickness of the fourth dielectric film 81 is preferably about 2 to 5 nm in order to obtain a CNR of 45 dB or more.
[Step 8] Nitriding treatment of magnetic film The medium after step 7 is subjected to nitriding treatment by introducing N 2 gas having a gas pressure of 1.0 Pa into the sputtering apparatus and leaving it at room temperature for about 5 minutes.
Here, although each magnetic film (5, 6, 7) is laminated | stacked on both the flat part and boundary part of a land-groove board | substrate, for example, since a boundary part is an inclined surface, each magnetic film The film thickness is thinner than the flat part. Further, the fourth dielectric film is not laminated at the boundary portion. Therefore, the magnetic film at the thin boundary portion (regions A and B in FIG. 2) is nitrided.
In addition, if the medium is exposed to an atmosphere of N 2 gas for an excessively long time, nitridation proceeds in a portion of the recording area that is not desired to be nitrided.
Therefore, the land-groove substrate land-to-groove boundary portion (inclined surface), the convex side wall surface of the groove substrate, or the concave side groove region of the land substrate may be left for a period of time that is nitrided. Since it is preferable, the leaving time is not limited to 5 minutes.
FIG. 3C shows a cross-sectional view after nitriding. By this nitriding treatment, the magnetic films (5, 6, 7) existing at the boundary portion between the land 21 and the groove 22 are nitrided to form nitride films 25, 26.
In the portions of the nitride films 25 and 26, magnetism has disappeared, so information cannot be recorded. Therefore, the magnetic films (5, 6, 7) on the flat portion of the adjacent land 21 and the flat portion of the groove 22 are magnetically separated by the nitride films 25, 26.
The magnetic film is composed of three layers (5, 6, 7). In order to magnetically separate the magnetic films in the adjacent recording areas, at least the third magnetic film 7 may be nitrided. Therefore, an appropriate standing time may be selected in consideration of the film thickness of the laminated magnetic films (5, 6, 7) and the fourth dielectric film 81, required recording characteristics, and the like.
[Step 9] Formation of third dielectric film 82 Target: Si
Sputtering gas: Ar gas, N 2 gas Flow rate ratio: Ar: N 2 = 2: 1
Gas pressure: 0.3Pa
Input power: 0.5 kW
Under the above conditions, SiN as the third dielectric film 82 is formed on the fourth dielectric film 81 to a thickness of about 53 nm. Here, the film thickness is not limited to 53 nm, but may be set so that the total thickness of the fourth dielectric film 81 is about 55 nm.
If the fourth dielectric film 81 is formed between 1 and 10 nm, the third dielectric film 82 may be formed at about 54 to 45 nm.
Through the above steps 1 to 9, the magneto-optical recording medium of the present invention as shown in FIG.
This forming process does not include a laser annealing process as in the past, and all processes except nitriding are reactive sputtering performed at room temperature, so the forming process can proceed smoothly and manufacturing costs can be reduced. can do. In addition, the regeneration characteristics are not deteriorated later as in the oxidation treatment, and the highly stable regeneration can be performed.
<Reproduction characteristics of magneto-optical recording media>
Next, the reproduction characteristics of the magneto-optical recording medium of the present invention will be described.
In order to examine the reproduction characteristics, the following evaluation experiment was conducted.
Evaluation apparatus: spectrum analyzer Optical system: objective lens NA = 0.85, wavelength 405 nm
Recording: Laser strobe magnetic field modulation recording method Recording frequency 50 MHz (= 0.15 μm)
Evaluation value: CNR (signal-to-noise ratio dB)
For comparison, in the conventional medium shown in FIG. 7, the third dielectric film 8 was formed without laser annealing of the magnetic film in the region not recorded after the formation of the third magnetic film 7 and laser annealing. Created something.
As a conventional medium subjected to laser annealing, a groove substrate and a land substrate were used, and as a conventional medium not subjected to laser annealing, three kinds of substrates including a land-groove substrate were used.
Further, in the conventional medium, the first dielectric film 2 to the third magnetic layer 7 formed on the substrate 1 are the same as the conditions shown in the steps 1 to 6 in the forming process of the present invention and the same. It was formed with a film thickness. The third dielectric film 8 was formed to have a film thickness of 53 nm under the same conditions as in Step 9.
In the case of performing laser annealing, laser annealing was performed by irradiating a region of the third magnetic layer 7 where recording was not performed with a high-power laser before the formation of the third dielectric film 8.
In the medium of the present invention, in order to confirm the effect of the nitriding treatment, the nitriding treatment time is fixed to 5 minutes, and the thickness of the fourth dielectric film 81 is changed from 1 nm to 10 nm in 1 nm units. Was created respectively.
FIG. 4 shows the CNR (dB) at the time of reproduction of the medium of the present invention when a land-groove substrate is used, FIG. 5 shows the CNR (dB) when a groove substrate is used, and FIG. CNR (dB) is shown. In either case, the horizontal axis represents the film thickness (nm) of the fourth dielectric film 81.
(A) Reproduction Characteristics of Land-Groove Substrate First, in the case of a land-groove substrate, a conventional medium not subjected to laser annealing does not cause domain expansion during reproduction because the domain wall is not separated, resulting in reproduction failure.
On the other hand, in the medium of the present invention, as shown in FIG. 4, when the thickness of the fourth dielectric film 81 is 1 nm and 10 nm, the CNR is about 37 dB, which is slightly bad, but in the range of 2 nm to 7 nm, the CNR = 42 to 46 dB, showing practical numerical values.
In particular, when the thickness of the fourth dielectric film 81 was 2 nm, CNR = 45.5 dB was shown, the magnetic domain was sufficiently expanded, and the effect of nitriding was the greatest.
If the film thickness of the fourth dielectric film 81 is about 1 nm or less, it is highly possible that the land and the flat portion of the recording area are also nitrided, so the CNR is considered to be low.
Further, when the film thickness is 10 nm or more, it is considered that the fourth dielectric film 81 is also laminated on the inclined surface that is the boundary portion between the land and the groove, and the nitriding treatment at this boundary portion is insufficient. It is considered that the separation of the magnetic film is incomplete and the CNR is lowered.
Therefore, in the case of a land-groove substrate, if an appropriate value in the range of 2 nm to 7 nm is selected for the thickness of the fourth dielectric film 81, stable domain expansion occurs during reproduction, and a practically good CNR can be obtained. it can.
(B) Reproduction characteristics of the groove substrate Next, in the case of the groove substrate, in the conventional medium not subjected to laser annealing, magnetic domain expansion during reproduction did not occur, resulting in reproduction failure.
In addition, the conventional medium subjected to laser annealing can be reproduced by expanding the magnetic domain, and the CNR was 43.0 dB.
On the other hand, in the medium of the present invention, as shown in FIG. 5, when the film thickness of the fourth dielectric film 81 was in the range of 2 to 5 nm, the CNR was higher than the CNR of the conventional medium. In particular, according to FIG. 5, when the film thickness was 3 nm, CNR = 46.0 dB, and the effect of nitriding was the greatest.
Therefore, also in the case of a groove substrate, if the film thickness of the fourth dielectric 81 of the medium of the present invention is appropriately selected, stable magnetic domain expansion occurs during reproduction, and a practically good CNR can be obtained.
(C) Reproduction characteristics of land substrate Next, in the case of a land substrate, in the conventional medium not subjected to laser annealing, magnetic domain expansion during reproduction did not occur, resulting in reproduction failure.
Further, in the conventional medium subjected to laser annealing, reproduction by magnetic domain expansion was possible, and the CNR was 42.5 dB.
On the other hand, in the medium of the present invention, as shown in FIG. 6, a CNR higher than the CNR of the conventional medium was obtained when the thickness of the fourth dielectric film 81 was in the range of 2 to 6 nm. In particular, according to FIG. 6, when the film thickness was 3 nm, CNR = 45.5 dB, and the nitriding effect was the greatest.
Therefore, in the case of a land substrate as well, if the film thickness of the fourth dielectric film 81 is appropriately selected, stable magnetic domain expansion occurs during reproduction, and a practically good CNR can be obtained.
As described above, in the magneto-optical recording medium of the present invention, after a dielectric film having a predetermined thickness is formed on the laminated magnetic film, a portion of the magnetic film that is not the information recording area is nitrided. Therefore, a practically good CNR can be obtained with stable reproduction characteristics.
Also, unlike the conventional media, there is no need for a laser annealing process, so the manufacturing process can be simplified and the manufacturing cost can be reduced, and the domain walls are separated by nitriding. A magneto-optical recording medium with more stable reproduction characteristics and no deterioration can be provided.
Furthermore, the medium having a laminated structure according to the present invention can be applied to a land-groove substrate, and can reduce the manufacturing cost and improve the reproduction characteristics in a high-density medium.

Claims (3)

基板上に、少なくとも放熱層を介して、それぞれ組成成分の異なる3層の第1,第2および第3磁性膜を積層し、これらの構造の上に所定膜厚の第4誘電体膜を形成した後、情報を記録しない領域の磁性膜を窒化させ、これらの構造の上に前記第4誘電体膜を構成する材料と同じ材料の第3誘電体膜をさらに積層させ、前記第3誘電体膜側から光を入射することにより情報を記録する光磁気記録媒体の形成方法であって、
前記基板が、表面に交互に複数個のランドおよびグルーブを形成した基板であり、隣接するランドとグルーブとの境界部分が傾斜面からなり、前記傾斜面が情報を記録しない領域であり、この傾斜面には前記第4誘電体膜が積層されない程度に第4誘電体膜がランドおよびグルーブ上の第3磁性膜の上に積層され、
基板上に、第1誘電体膜、放熱層、第2誘電体膜をこの順に積層する第1工程と、前記第2誘電体膜の上に、第1磁性膜と、第1磁性膜よりもキュリー温度の低い第2磁性膜と、第1磁性膜よりも磁壁抗磁力が低く、かつ第2磁性膜よりもキュリー温度の高い第3磁性膜とをこの順に積層する第2工程と、前記第3磁性膜の上に、所定膜厚の第4誘電体膜を積層する第3工程と、情報を記録しない領域の前記第3磁性膜を少なくとも窒化させる第4工程と、窒化された前記第3磁性膜および第4誘電体膜の上に、前記第3誘電体膜を積層する第5工程とをこの順に実施することを特徴とする光磁気記録媒体の形成方法。
Three layers of first, second, and third magnetic films having different composition components are laminated on a substrate via at least a heat dissipation layer, and a fourth dielectric film having a predetermined thickness is formed on these structures. Then, a magnetic film in a region where no information is recorded is nitrided, and a third dielectric film made of the same material as that constituting the fourth dielectric film is further laminated on these structures, and the third dielectric A method of forming a magneto-optical recording medium for recording information by entering light from a film side ,
The substrate is a substrate in which a plurality of lands and grooves are alternately formed on the surface, a boundary portion between adjacent lands and grooves is an inclined surface, and the inclined surface is an area where information is not recorded, and this inclined A fourth dielectric film is laminated on the third magnetic film on the land and the groove to such an extent that the fourth dielectric film is not laminated on the surface;
A first step of laminating a first dielectric film, a heat dissipation layer, and a second dielectric film in this order on a substrate; and a first magnetic film and a first magnetic film on the second dielectric film. A second step of laminating a second magnetic film having a low Curie temperature and a third magnetic film having a domain wall coercive force lower than that of the first magnetic film and having a Curie temperature higher than that of the second magnetic film in this order; A third step of laminating a fourth dielectric film having a predetermined thickness on the three magnetic films, a fourth step of nitriding at least the third magnetic film in a region where information is not recorded, and the nitrided third step A method of forming a magneto-optical recording medium , comprising: performing a fifth step of laminating the third dielectric film on the magnetic film and the fourth dielectric film in this order .
基板上に、少なくとも放熱層を介して、それぞれ組成成分の異なる3層の第1,第2および第3磁性膜を積層し、これらの構造の上に所定膜厚の第4誘電体膜を形成した後、情報を記録しない領域の磁性膜を窒化させ、これらの構造の上に前記第4誘電体膜を構成する材料と同じ材料の第3誘電体膜をさらに積層させ、前記第3誘電体膜側から光を入射することにより情報を記録する光磁気記録媒体の形成方法であって、
前記基板が、表面に複数個のグルーブを形成した基板であり、隣接するグルーブの境界部分が凸形状の側壁面から構成され、前記側壁面が情報を記録しない領域であり、この側壁面には前記第4誘電体膜が積層されない程度に、第4誘電体膜がグルーブ上の第3磁性膜の上に積層され、
基板上に、第1誘電体膜、放熱層、第2誘電体膜をこの順に積層する第1工程と、前記第2誘電体膜の上に、第1磁性膜と、第1磁性膜よりもキュリー温度の低い第2磁性膜と、第1磁性膜よりも磁壁抗磁力が低く、かつ第2磁性膜よりもキュリー温度の高い第3磁性膜とをこの順に積層する第2工程と、前記第3磁性膜の上に、所定膜厚の第4誘電体膜を積層する第3工程と、情報を記録しない領域の前記第3磁性膜を少なくとも窒化させる第4工程と、窒化された前記第3磁性膜および第4誘電体膜の上に、前記第3誘電体膜を積層する第5工程とをこの順に実施することを特徴とする光磁気記録媒体の形成方法。
Three layers of first, second, and third magnetic films having different composition components are laminated on a substrate via at least a heat dissipation layer, and a fourth dielectric film having a predetermined thickness is formed on these structures. Then, a magnetic film in a region where no information is recorded is nitrided, and a third dielectric film made of the same material as that constituting the fourth dielectric film is further laminated on these structures, and the third dielectric A method of forming a magneto-optical recording medium for recording information by entering light from a film side,
The substrate is a substrate in which a plurality of grooves are formed on the surface, and a boundary portion between adjacent grooves is constituted by a convex side wall surface, and the side wall surface is a region in which information is not recorded. The fourth dielectric film is laminated on the third magnetic film on the groove to the extent that the fourth dielectric film is not laminated,
A first step of laminating a first dielectric film, a heat dissipation layer, and a second dielectric film in this order on a substrate; and a first magnetic film and a first magnetic film on the second dielectric film. A second step of laminating a second magnetic film having a low Curie temperature and a third magnetic film having a domain wall coercive force lower than that of the first magnetic film and having a Curie temperature higher than that of the second magnetic film in this order; on the third magnetic film, a third step and a fourth step of at least nitriding said third magnetic film in the region that does not record information, the third nitrided for laminating the fourth dielectric film having a predetermined thickness on the magnetic film and the fourth dielectric film, forming method of the magneto-optical recording medium and a fifth step which comprises carrying out in the order of laminating the third dielectric film.
前記第4工程が、第4誘電体膜を積層した後の媒体を、室温かつ窒素雰囲気中に所定時間放置することで行われることを特徴とする請求項1または2の光磁気記録媒体の形成方法。Formation of the fourth step, the fourth medium after the dielectric layer is deposited, according to claim 1 or 2 of the magneto-optical recording medium characterized in that it is carried out is left for a predetermined time in room temperature and nitrogen atmosphere Method.
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